romiogY Vol. 2, pp. 299-340. Pcrgamon Press. 1963. Printed in Great Brimin MORSE THEORY ON HILBERT ~ANrF~LDS RICHARD S. PALAIS THE TERM “MORSE THEORY' is usually understood to apply to two analagous but quite distinct bodies of mathematical theorems. On the one hand one considers a smooth, real valued functionfon a compact manifold M, defines M, = f - ‘[ - x), a], and given a closed interval [a, 61 describes the homology, homotopy, homeomorphism or diffeomorphism type ofthe pair (Mb, M,) in terms of the critical point structure off in f-‘[a, b]. On the other hand one takes a compact Riemannian manifold V, defines M to be the ‘loop space’ of piecewise smooth curves joining two points (with a natural topology) and f: N -+ R the length function and again describes the homology and homotopy type of (Mb, M,) in terms of the critical point structure offinf-‘[a, 61 (i.e. in terms of the geodesics joining the two points whose Iengths lie between a and b). The classical approach to this second Morse theory is to reduce it to the first Morse theory by approximating M, (up to homotopy type) by certain compact submanifolds of piecewise broken geodesics. A particularly eIegant and lucid exposition of this cfassical approach can be found in John Milnor’s recent Annals Sri&y [S]. Our goal in the present paper is to present a Morse theory for differentiable real valued functions on Hilbert manifolds. This encompasses both forms of Morse theory mentioned above in a unified way. In addition the generalization of the Morse theory of geodesics to higher loop spaces (i.e. maps of an n-disk into a manifold with fixed boundary conditions) and even more general situations works smoothly in th.is framework, whereas previous attempts at such generalizations were thwarted by the lack of a good analogue of the approximating compact manifolds of piecewise broken geodesics. We have endeavored to make the exposition relatively self contained. Thus the first two sections give a brief resume of the classical theory of Frechet on the differential calculus of maps between Banach spaces (details and proofs will be found in [I]) and in sections 3 to 9 we give a brief treatment of the theory of Banach manifolds with particular emphasis on Hilbert manifolds (details and proofs will be found in [4]). In sections 10 through 12 we prove the MAIN THEOREM OF MORSE THEORY Let M be a complete Riemannian manifold of class C.“’ (k > I) and f: M + R a C”“‘-function. Assume that all the critical points offare non-degenerate and in addition
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romiogY Vol. 2, pp. 299-340. Pcrgamon Press. 1963. Printed in Great Brimin
MORSE THEORY ON HILBERT ~ANrF~LDS
RICHARD S. PALAIS
THE TERM “MORSE THEORY' is usually understood to apply to two analagous but quite distinct
bodies of mathematical theorems. On the one hand one considers a smooth, real valued
functionfon a compact manifold M, defines M, = f - ‘[ - x), a], and given a closed interval
[a, 61 describes the homology, homotopy, homeomorphism or diffeomorphism type ofthe pair
(Mb, M,) in terms of the critical point structure off in f-‘[a, b]. On the other hand one
takes a compact Riemannian manifold V, defines M to be the ‘loop space’ of piecewise
smooth curves joining two points (with a natural topology) and f: N -+ R the length
function and again describes the homology and homotopy type of (Mb, M,) in terms of the
critical point structure offinf-‘[a, 61 (i.e. in terms of the geodesics joining the two points
whose Iengths lie between a and b). The classical approach to this second Morse theory is
to reduce it to the first Morse theory by approximating M, (up to homotopy type) by
certain compact submanifolds of piecewise broken geodesics. A particularly eIegant and
lucid exposition of this cfassical approach can be found in John Milnor’s recent Annals
Sri&y [S].
Our goal in the present paper is to present a Morse theory for differentiable real
valued functions on Hilbert manifolds. This encompasses both forms of Morse theory
mentioned above in a unified way. In addition the generalization of the Morse theory of
geodesics to higher loop spaces (i.e. maps of an n-disk into a manifold with fixed boundary
conditions) and even more general situations works smoothly in th.is framework, whereas
previous attempts at such generalizations were thwarted by the lack of a good analogue of
the approximating compact manifolds of piecewise broken geodesics.
We have endeavored to make the exposition relatively self contained. Thus the first
two sections give a brief resume of the classical theory of Frechet on the differential calculus
of maps between Banach spaces (details and proofs will be found in [I]) and in sections
3 to 9 we give a brief treatment of the theory of Banach manifolds with particular emphasis
on Hilbert manifolds (details and proofs will be found in [4]).
In sections 10 through 12 we prove the
MAIN THEOREM OF MORSE THEORY
Let M be a complete Riemannian manifold of class C.“’ (k > I) and f: M + R
a C”“‘-function. Assume that all the critical points offare non-degenerate and in addition
300 RICHARD S. PALAIS
(C) If S is any subset of Mon whichf is bounded but on which /I Vfll is not bounded
away from zero then there is a critical point off adherent to S. Then
(a) The critical values off are isolated and there are only a finite number of critical
points off on any critical level;
(b) If there are no critical values offin [a, b] then Mb is diffeomorphic to M,,;
(c) If c c c < b and c is the only critical value offin [a, 61 and pi, . . ., p, are the critical
points off on the level c, then Mb is diffeomorphic to M, with r handles of type (k,, I,),
. ..( (k,, I,) disjointly CL-attached, where ki and li are respectively the index and co-index
Of pi.
It should be noted that iffis proper, i.e. iff-‘[a. 61 is compact for every closed interval
[u, b], then condition (C) is automatically satisfied, hence the Morse theory for compact
manifolds is included in the above theorem. On the other hand if M is infinite dimensional,
hence not locally compact, then it is impossible for a real-valued function f: M + R to
be proper whereas we shall see condition (C) is still satisfied in cases of significant interest.
A theorem similar to the above was obtained independently and essentially simul-
taneously by S. Smale.
In $13 we show how to interpret the loop space of a complete finite dimensional
Riemannian manifold V as a complete infinite dimensional Riemannian manifold M.
This is due to Eells 121, however we have followed an approach suggested by Smale. In
$14 we show that if we take f: M + R to be the ‘action integral’ then the hypotheses of
the Main Theorem are satisfied, thereby deriving the Morse theory of geodesics. In $15
we return to the abstract Morse theory of functions satisfying condition (C) on a Riemannian
manifold and in particular derive the Morse inequalities. Finally in $16 we comment
briefly on generalizing the Morse Theory of geodesics to higher loop spaces, a subject we
hope to treat in detail in a later paper.
41. DIFFERElVl-LUILITY
Let V and W be Banach spaces, 8 an open set in V and f: 0 -+ W a function. If
p E 0 we say that f is differentiable at p if there exists a bounded linear transformation
T: V + W such that /f(p + x) -f(p) - TX ]l/]l )] x - 0 as x -+ 0. It is easily seen that
T is uniquely determined and it is called the differential off at p. denoted by dfp. The
following facts are elementary [l, Ch. VIII]:
Iff is differentiable at p then f is continuous at p;
Iffis differentiable at p and U E 8 is a neighborhood ofp then g = f 1 U is differentiable
at p and dgp = df, ;
Iffis constant then it is differentiable at p and d& = 0;
If S : V --* W is a bounded linear transformation and _f = S]8 then f is differentiable
at p and df, = S;
If f is differentiable at p, g : 0 + W is differentiable at p and z, /I are real numbers
then (zf + pg) is differentiable it p and d (zf + /?g), = adf, + /?dg,;
MORSETHEORY OK WLBERT MA~-lFOLDS 301
If U is a neighborhood off@) and g : U + Z is differentiable at_@) then iffis differ- entiable at p, g qf is differentiable at p and d(g 3f)p = dgft,, D df,.
Now suppose f is differentiable at each point of 8. Then df: p -+ d& is a function from 8 into the Banach space L(V, W) of bounded linear transformations of Y into W (sup. norm). If df is continucrus then we say thatjis of class C’ in 0. If dfis differentiable at a point p E B then d(df), = d’jfp E L(K L(V, W)). We make the usual canonical identification of L(V, L(V, W)) with L2(Vs W), the space of continuous bilinear maps of V x V into W. Thus d2fP is interpreted as a bilinear map of V x V into W and it can easily be shown to be symmetric ]l, p. 1751. In case d’& exists at each p E 0 and the map d2f: p -f d2fP is continuous we say that f is of class C2 in 0. Inductively suppose dkf: 0 I* S’(V, W) exists and is differentiable at p. Then (d’” tf>, = d(dy), E
L( V, tk( V, W)) z Lk+‘( V, W) and dkflfp. the (k + I)st differential offat pY is a bounded, symmetric [ 1, p, 1761 (k + 1).linear map of V x .,. x V into W. If d”ifP exists at each pointpEIIanddk”‘f:@-+L k’ ‘( V W) is continuous then we say that f is of class Ckfl in 0. Iffis of class C’ in 0 for ever; positive integer k we say thatfis of class C” in 0.
A linear map of R into a Banach space W is completely determined by its value on the basis element 1. We use this fact to define the derivative of a differentiable function f‘: 19 -+ W where 0 2 R: namely the derivative off at p, denoted by J’(p)+ is defined by f’(p) = df,(l)% so d&(a) = af’(p). If f is differentiable at each point of 0 we have f ’ : U -+ W, and if f is of class C’ in 0 we can define f ” = (f ‘)’ and in generai if f is of class CL we can define f (kf : Q --t W. Clearly the relation off”’ and dLfis dk&(,<t, . . . . XJ = xix2 . . . M”(*YP). If g : W + Z is differentiable then (g Olf)‘tpj = d(g Qf),(I) =
dg~~~~(d~(l~~ = d~~,~~~ff~~~, i.e. (9 of)' = dsI cf'. For future reference we note the following. If B is a continuous symmetric bilinear map
of Y x V into FV thenf: Y + W defined byfi:n) = B(G’, v) is of class C”. In fact d&(u) I = 2B(p, mu). d’f = ZB and d’f = 0.
,_ . . St. THREE BASIC THEOREMS
Let V and W be Banach spaces, p E V, 0 a convex neighborhood of p in V andf : Q -+ W a Ck-map, k r 1. Then there is a CL-‘-map R, : S-+L(V, W).such that 1yx =p + ve8
f(x) =f(p) + R,(x)c.
COROLLARY (TAYLOR'S THEOREM). If m I k there is a Ck-mwmap R, :cI1 + Lm( V, W) such that ifx = p + v E: 0 then
La V and W be ~li&ueh spaces, 0 open in V, and f : 0 + W a Cc-map, k L I. Let p E B and suppose that dfF mops V me-m-me mm W. Then there is a neighborhood U of
302 RICHARD S. PALAIS
p included in B such that f 1 U is a one-to-one map of U onto a neighborhood of f(p) and more-
over (f I V)- I is a Cc-map off(U) onto U.
DEFINITION. If 8 is an open set in a Banach space V then a C’-vector jietd in 0 is a
C’map X: B + V. A solution curve X is a Cl-map o of an open interval (a, b) E R into r?
such that o’ = X 0 CT. If 0 E (a, b) we call a(O) the initial condition of the sohaion a.
The following theorem is usually referred to as the local existence and uniqueness
theorem for ordinary differential equations (or vector fields).
THEOREM. Let X be a CL-vector field on an open set 0 in a Banach space V, k 2 1.
Given p. E 0 there is a neighborhood U of p. included in 0, an E > 0, and a CL-map
q : U x (- E, E) --) V such that:
(1) Ifp E U then the map op : (-E, E) + V defined by a,(t) = cp@, t) is a solution of
X with initial condition p:
(2) If u : (a, b) --* V is a solution curve of X with initial condition p E U then a(r) =
a,(t) for It] < E.
The proofs of these three basic theorems can all be found in [l] or in [4].
$3. DIFFEREF44LX MANIFOLDS WITH BOUNDARY
If k is a bounded linear functional on a Banach space V, k # 0 we call H=
{v E V(k(v) 1 0) the (positive) half space determined by k, and dH = {v E V(k(v) = O> is
called the boundary of H. A function f mapping an open set 0 of H into a Banach space U’
is said to be of class CL at a point p E 0 n dH if there exists a C’-map g : U -+ W, where U
is a neighborhood ofp in V, such that f (0 n U = gj8 n V. It is easily seen that d”f, = dmg,
is then well defined for m I k and that iffis of class C’ at each point of 0 n 8H and also in
0 - 8H then d*f: 0 + L”(V, W) is continuous for m 5 k; in this case we say that f is of
class Ck in 0. Next suppose that f is a one-to-one Ck-map of 0 into an open half space
K in W. We say that f is a Ck-isomorphism of 0 into K if f(S) is open in K and iff -i is of
class CL (if k 2 1 then it follows from the inverse function theorem that this will be so if
and only if dfP maps V one-to-one onto W for each p E 0).
Invariance of Boundary Theorem
Let H, be a half space in a Banach space V, and 0, an open set in H, (i = 1,2). Let
f : 0, + O2 be a C’-isomorphism. Then tf- either k 2 1 or dim Vi < co f maps 8, n aH,
Ck-isomorphically onto O2 n dH,.
Proof. In case k 2 1 the result is an immediate consequence of the inverse function
theorem. In case dim Vi < cg the theorem follows from invariance of domain.
Caution. In case k = 0 and dim V, = 00 the conclusion of the theorem may well fail.
Thus if V is an infinite dimensional Hilbert space and H a half space in V it is a (non-
trivial) theorem that H and H - dH are homeomorphic.
MORSE THEORY ON HILBERT MANIFOLDS 303
In the following, to avoid logical difficulties, we shall fix some set S of Banach spaces
and whenever we say Banach space we will mean one which belongs to the set S.
A chart in a topological space X is a homeomorphism of an open set D(cp) of X onto
either an open set in a Banach space or else onto an open set in a half space of a Banach
space. Two charts p and $ in X. with U = D(q) n D(G). are called CL related if $ O cp-’
is a Ck-isomorphism of q(U) onto t,b(U). A C’-atlas for X is a set ri of pairuise C’-related
charts for X whose domains cover X, and A is called complete if it is not included in any
properly larger CL-atlas for X. It is an easy lemma that if each of two charts cp, $ in X
is Ck-related to every chart in A then cp and li/ are CL-related. It follows that there is a
unique complete C’-atlas 1 including A. namely the set of all charts cp in X such that 43
is Ck-related to every chart in A, A’ is called the completion of A.
A CL-manifold with boundary is a pair (X, A) where X is a paracompact Hausdorff
space and A is a complete CL-atlas for X. In general we will use a single symbol, such as
.M. to denote both a C’-manifold (X, A) and its underlying topological space X, and
elements of A will be referred to as charts for M. If p E M a chart at p is a chart for M
having p in its domain. If A is a (not necessarily complete) CL-atlas for X then by the
C’-manifold determined by A we mean the pair M = (X, 2). If m < k then A is a Cm-atlas
for X and so determines a Cm-manifold which we also denote by ,ti (an abuse of notation),
so that a Ck-manifold is regarded as a Cm manifold if m I k.
If M is a C’-manifold, k 2 1, we define dA4 to be the set of p E A4 such that there exists
a chart cp at p mapping D(q) onto an open set in a half space H so that p(p) E dH. It
follows from the invariance of boundary theorem that every chart at p has this property
and also that {cp[aM}, where cp runs over the charts for M, is a C’-atlas for iiM, so dM is
a C*-manifold. Moreover we have the obvious, but satisfying relation ;I(aM) = 4,
If M and N are C’-manifolds a functionf: IV -+ N is said to be of class CL near p if
there exists a chart cp at p and a chart 1(1 at&) such that (i/ Of 5 9-l is of class CL, and fis
said to be of class C’ if the latter holds for each p E M. It is easily seen that f: ,U_ + N is of class C” if and only if $ 3 f 3 cp -' is C’ for every chart cp for iii and $ for N.
If we define objects to be C’-manifolds and morphisms to be P-maps then the axioms
for a category are satisfied.
84. TANGEh-T SPACES AND DIFFERENTIALS OF IMAPS
Let {Vi];;, be an indexed collection of Banach spaces and for each (ij) E Z* let cpij
be an isomorphism of V’j with Vi (as topological vector spaces) such that cpii = identity
and cpuqjk = ~ik. From the data {Vi, vii} we construct a new Banach space Y (by a
process we shall call amalgamation) and a canonical isomorphism ILi : V -+ Vi such that
rri = pijnj. Namely V is the set of {oi} in the Cartesian product of the Vi such that
Ui = VijUj. Clearly V is a subspace of the full Cartesian product, hence a topological vector
space. We define rri to be the restriction of the natural projection of the Cartesian product
onto V,. To prove that V is a Banach space and n, an isomorphism it suffices to note that
there is an obvious continuous, linear. two sided inverse 1, to rrj, namely Ij(v)i = cp,,(u).
304 RICHARD S. PALMS
Given a second set of data {IV,, +t,} satisfying the same conditions (with indexing
set K) suppose that for each (i, k) E I x K we have a bounded linear transformation
Tki : Vi + W’k such that \I/~ITri’pij = Tk,. Then if W is the amalgamation of {W,, +,..I
there is a uniquely determined bounded linear map T: V -, W such that n,T = T,JK~.
namely if {vi} E V then T {ci} = {We} where tipt = Tkici. T is called the amalgamation of
the T,,.
Now suppose M is a C’-manifold k 2 1, p E M and let I be the set of charts at p.
Given cp E I let V,,, be the target of cp (i.e. the Banach space into which cp maps D(p)). Then
for each (cp, $) E 1’ d($ O v-‘)~~~) is an isomorphism of I’,+, onto V,. Clearly d(ip O (P-‘)~,~)
= identity and by the chain rule d(f. d (p-1)0(p) O d(rp O $-l)+(,,) = d(l ., +-‘)40,,. Hence
the conditions for an amalgamation are satisfied. The resulting amalgamation is called
the tangent space to M at p and denoted by M,.
Let N be a second C’-manifold f: M + N a C’-map and K the set of charts at f(p). For each (cp, $) E I x K we have a linear map d($ Of o 'p-')+,(,,) of V, into W+. Moreover
the abstract condition for amalgamating is clearly satisfied, hence we have a well determined
amalgamated map dfP : M, 4 Nftpj called the differential off at p,
$5. THE TANGENT BUNDLE
Let n : E -+ B be a CL map of Ck-manifolds and suppose for each b E B n-‘(b) = Fb
has the structure of a Banach space. We call the triple (E, B, x) a Ck-Bunach space bundle
if for each b,, E B there is an open neighborhood U of b. in B and a C’-isomorphism
f:Ux Fbozn - ‘(U) such that u + f(b, u) is a linear isomorphism of F,, onto Fb for each
b E U. If (E’, B’, n’) is a second C’-Banach space bundle then a CL-map f: E + E’ is
called a C’-bundle map if for each b E B f maps Fb linearly into a fiber FYfb,. The map
f : B -+ B’ is then CL and is called the map induced by J
Let M be a CL+ l-manifold with boundary. Let T(M) = ,yM M, and define
II : T(M) + M by n(M,) = p. Given a chart cp for M with domain U and target V,
define cp : U x V, -+ n- '(U) by letting u -+ cp(p, v) be the natural isomorphism of I’,
with M,. Then it is a straightforward exercise to show that the set of such cp is a CL-atlas
for a CL-manifold with underlying set T(M) and moreover that T(M) is a Ck-Banach space
bundle over M with projection II. Iff is a C’+ ‘-map of M into a second C’+ i-manifold N
we define df: T(M) -* T(N) by df lA4, = dfP. Then one shows that df is of class Ck and
is a bundle map which clearly has f as its induced map.
The category whose objects are C’-Banach space bundles and whose morphisms are
CL-bundle maps is called the category of CL-Banach space bundles. The function M + T(M),
f --* df is then a functor from the category of Ck+ ’ -manifolds with boundary to the category
of C’-Banach space bundles. Since each author has his own definition of the tangent
bundle functor it is useful to have a general theorem which proves they are aLl naturally
equivalent, i.e. a characterization of T up to natural equivalence in purely functorial terms.
To this end we first note two facts. If 0 is an open subset of a CL-manifold M then 0 is in
MORSE THEORY ON HILBERT MASIFOLDS 305
a natural way a C’-manifold called an open submanifold of M: namely a chart for 0 is a
chart for M whose domain is included in G. If M is a 3anach space V or else a half space
in a Banach space V then the identity map of M is a chart in M and its unit class is a C” r- atlas for M. The Ckfl-manifold defined by this atlas will also be denoted by M. The
corresponding full subcategory of the category of Ckf ’ -manifolds with boundary which
we get in this way will be referred to as the subcategory of Banach spaces and half spaces.
On this subcategory we have an obvious functor T into the category of Ck-Banach space
bundles; namely with each such CL+’ -manifold M we associate the product bundle
r(M) = M x V considered as a Ck-Banach space bundle, and iff: M -+ N is a CL+ ‘-map.
where N is either a Banach space W or else a half space in W, then the induced map
r(f) : M x V --* N x W is given by r(f)(m, I’) = (f(m), dfm(r)). We now characterize
the notion of a tangent bundle functor.
DEFINITION. A functor t from the category of C”’ -manifolds to the category of C”-
Banach space bundles is called a tangent bundle functor if
(1) t(M) is a bundle over M and tff : M -+ N then f is the induced map of t( f ),
(2) Restricted to the subcategory of Banach spaces and halfspaces t is naturally equivalent
to 5,
(3) If M is a C’+’ -mantfold and 0 is an open-submantfold and 1 : 0 -+ M rhe inclusion
map then t(8) = t(M)10 and t(1) is the inclusion of f(0) in t(M).
THEOREM. The functor T defined above is a tangent bundle finctor. Moreover any two
tangent bundle,functors are natural1.v equivalent.
46. INTEGRATION OF VECTOR FIELDS
Leta:(a,b)+MbeaC’+’ -map of an open interval into a CA+‘-manifold M. We
define a Ck-map 6’ : (a, 6) -+ T(M), called the canonical lifting of 6, by a’(r) = da,(l).
We note that rcc’ = G i.e. that 6’ is in fact a lifting of 0.
DEFINITION. A CL-vector field on a Ck+ ’ -manifold M is a CL-cross section of T(M),
i.e. a CL map X: M -+ T(M) such that TC 0 X = identity. A solution curve of X is a Cl-map
u of an open interval into M such that cr’ = X 0 CT. If 0 is in the domain of the solution u w’e
call u(0) the initial condition of the solution a.
The facts stated below are straightforward consequences of the local existence and
uniqueness theorem for vector fields and proofs will be found in [4, Chapter IV].
Let M be a CL+‘-manifold (k 2 1) with dM = 4 and let X be a CL-vector field on M.
THEQREM (1). For each p E M there is a solution curve aP of X with initial condition p
such that every solution curve of X with initial condition p is a restriction of CT,.
The solution curve up in the above theorem is called the maximum solution curve of X
with initial condition p. We define t+ : M+(O,co]andt-:M+[-co,O)bytherequire-
ment that the domain of u,, is (l-(p), t’(p)). They are called respectively the positive and
negative escape time functions for X.
306 RICHARD 5. PALAIS
THEOREM (2). [‘t-(p) c s c t’(p) and 9 = a,(s) then a,, = op O T, where 5, : R 4 R
is defined by 5,(t) = s + t. In purticufur t+(9) = t’(p) - s and t-(9) = t-(p) - s.
THEOREM (3). tC is upper semi-continuous and t - is lower semi-continuous. Also if
t+(p) < co then a,(t) has no limit point in M as t -+ t’(p) and if t-(p) > -XI then a,(t)
has no limit point in M us t - t-(p).
COROLLARY. If M is compuct then tf E co and t- = -a .
To state the final and principal result we need the notion of the product of two CL-
manifolds. This is defined if at least one of the two manifolds has no boundary. If
c~ : D(p) +. V is a chart for M and tj : D(9) --+ W is a chart for N then cp x $ : D(p) x
D(l(/) + V x W is a chart in M x N (note that the product of a half-space in I’ with W
is a half-space in V x W). The set of such charts is a C’-atlas for M x N and we denote
by M x N the resulting Ck-manifold. If N has no boundary then Z(M x N) = (dM) x N.
Now we go back to our C’-vector field X on a C” ‘-manifold M with ZM = 4.
DEFINITION. Let D = D(X) = {(p, t) E M x Rlt-(p) < t < t’(p)} and for each
t E R let D, = D,(X) = {p E Ml(p, f) E D). Define cp : D -+ M by cp@, t) = a,(t) and
cPr. . D, -+ A4 by qr(p) = o,(t). The indeex-ed set q, is culled the maximum local one parameter
group generated by X.
THEOREM (4). D is open in M x R and cp : D + M is of class C’. For each t E R D, is
open in M and qr is u Ck-isomorphism of D, onto D_ t hucing cp- f us its inverse. If p E D,
andq,,(p)E D, thenp E D,+,undcp,+,(p) = CP~(CP,(P)).
$7. REGULAR AND CRITICAL POINTS OF FUNCTTONS
Let M be a C’-manifold, f: M + R a CL-function. If p E M then df, is a bounded
linear functional on Mp, If dfp # 0 then p is called a regular point off and if df, = 0 then
p is called a critical point off. If c E R thenf- ‘(c) is called a level off (more explicitly the
c-level off) and it is called a regular level off if it contains only regular points off and a
critical level off if it contains at least one critical point off. Also we call c a regular value
off iff -l(c) is regular and we call c a critical value off iff -l(c) is critical.
If f and M are C2 then there is a further dichotomy of the critical points off into
degenerate and non-degenerate critical points. We consider this next.
LEMMA. Let q be u Ck-isomorphism of an open set 0 in a Eunuch space V onto an open
set 0’ in a Bunach space V’ (k 2 2). Letf: 0’ +RbeofclussC2andletg=fOcp:O+R.
Then if dg, = 0, d’g,(o,, 0J = d’f&,(drp,(uJ, dqp(t’2)).
hence G’(x) = df ft,,G’(x) df+(=,, x E U. Since f is of class C’+’ it follows that if G’ is of
class CL in I/ then so also is G’. Hence it is consistent to demand for each chart Q, that GQ
is of class CL. If this is so we will call x --, (,), a CL Riemannian structure for M, and M
equipped with this extra structure will be called a Ckfl-Riemannian manifold. We will
MORSE THEORY ON HILBERT MANIFOLDS 311
maintain the notation used above. That is given a chart cp in a Ck-Riemannian manifold
M we will denote by G” the function defined above, and in addition we define R+’ on
D(p) by P(x) = (G’(x))-‘. Also we define a function *I / in T(M) by “c;; = (r, r)‘;’
for u E M,,. Clearly ‘i 1,’ is of class CL on T(M), hence ! :, is continuous on T(M) and of
class C’ on the complement of the zero section. If cr : [a, h] -+ M is a Cl-map then
t + iiu’(t);/ is continuous on [a, b] hence
L(a) = ‘,,o’(t)!, dr J 0 is well defined and is called the length of 0. It is easily seen that if x and )’ are two points
in the same component of M then there exists a C’-curve joining them, hence we can define
a metric p in each component of M by defining p(x, y) to be the infimum of the lengths of
all Cl-paths joining x and y. It is clear that p is symmetric, satisfies the triangle inequality,
and is non-negative. That p(x, ~1) > 0 if x # )’ and is hence a metric, and that the topology
given by this metric is the given topology of M follows easily from the following two lemmas:
LEMMA (1). Let H be a Hilbert space, f: [a, b] - H a C’-map. Then
J b
llf’(f)ii dt 2 iIf(b) -f(a)il. *
Proof. We can suppose f(b) # f(a). Let g(t)(f(b) - f(a)) be the orthogonal projection
off(t) -f(a) on the one-dimensional space spanned by f(h) -f(a). Then g : [a. h] -+ R
is C’, g(a) = 0, g(b) = 1 and f(t) -f(a) = g(t)(f(b) -f(a)) + h(t) where h : [a, h] -+
(f(b) -f(a))’ is C’. Then f’(t) = g’(tKf(b) - J(a)) + h’(t) where h’(t) 1 (f(b) - f(a)).
hence
so
llf’(t)l~* = :,.f(b) -f(a~i~*~ld(Ol* + W(t)ll* L ll,f(hl -
But
Ilf’(~)il dt 2 Ill(b) -./‘(ahi . J b
k ([Ii dt. a
q.e.d.
LEMMA (2). Let H be a Hilbert space, p E H, and G a continuous map of a neighborhood
of p into the space of posirive operators on H. Then there exists r > 0 such rhat G is d@ined
on B,(p) and positire constants K and L such that.
(1) yf: [a, b] + B,(p) is a Cl-map withf(a) = p
312 RICHARD S. PALAIS
(2) iff: [a, b] + His a C’-map withf(a) = p and c = Sup {t E [a, b]]f([a, r]) c B,(p)}
then
s c(c(f(t))f’(t),j’(t))lIZ dt > Lr. a
Proof Let Q(x) = G(x)-‘. By continuity of G and Q we can choose K and L > 0
such that liG(x)ll < K2 and liQ(x)ll < Le2 for x in some open ball B,@). Then
(G(f(r))f’(r)9f’(r)> S K’U’(r)>f’(r)> and
(f’(r)J’(r)> = Wf(r))G(f(r))f’(r)J’(r))
I L- 2<G(f(r))f’(r)7 f’(r)>
if f(r) E B,(p). Then (1) follows immediately while (2) follows from (1) and Lemma (1). q.e.d.
DEFINITION. rf M is a Ck+’ -Riemannian manifold then the metric p defined above on
each component of M is called the Riemannian metric of M. If each component of M is a
complete metric space in this metric then M is called a complete C” ‘-Riemannian manifold.
If’b is a Cl-map of an open interval (a, b) into a Riemannian manifold M we define the
length of Q, L(a),,to be
lim ‘/a’(r)l\ dr. i (1-o ;I
B-b
Of course L(a) may be infinite. However suppose L(a) < co. Given E > 0 choose t, = a < t, < . . . < t, c b = tn+l so that
ft+ I [la’(t)jl dt < E.
li
Then clearly a((a, 6)) is included in the union of the s-balls about the a(t,) i = 1, 2, . . . . n.
Thus
PROPOSITION (1). Zf M is a C’+ ’ -Riemannian manifold and o : (a, b) + M is a Cl-curve
of finite length, then the range of CT is a totally bounded subset of M, hence has compact
closure if M is complete.
PRORXITION (2). Let X be a Ck-vector field on a complete Ckf ‘-Riemannian manifold
M(k 1 1) and let cr : (a, b) -+ M be a maximum solution curve of X. If b c co then
I
b
II-WWI dt = 00 0
(in particular [/X(17(t)) I( is unbounded on [O, b)) and similarly if a > - co then
I ollX(o(t))/l dt = 00
(in particular [lX(u(t)) // is unbounded on (a, 01).
MORSE THEORY ON HILBERT MAhIFOLDS 313
Proof. Since a’(t) = X(a(t)) it follows from Proposition (1) that if
s
b
llX(d4>ll dl < ~0 0
then a(t) would have a limit point as t --+ b, contradicting Theorem (3) of $6. q.e.d.
Now letf: M -+ R be a CL+’ real valued function on a Ckf ‘-Riemannian manifold M.
Given p EM df, is a continuous linear functional on )%I,, hence there is a unique vector
Vf, E M, such that dfp(r) = (L., Vf,), for all L‘ E iv,. Vfp is called the gradient off at p and Vf: p --) Vf, is called the gradient off. We claim that Vf is a CL-vector field in M.
To prove this we compute it explicitly with respect to a chart p : D(q) + H where H is a
Hilbert space with inner product, (,). Let T be the canonical identification of H* with
H, so if I E H* then I(c) = (L., Tl). Since T is a linear isomorphism it is C”. Define g on
the range U of c~ by g = f 3 c+o-l. Then g is of class Ckr ’ hence dg : Cl -* H* is class C’
Recalling the inequality (u, Q(x)u) 2 /jG(x)/j-’ . ~Iu/\~
(V/U- P)(X) 2 8iKp - Oxll(ll(P - Ox-ll.liG(x)li-’ - i/~ll~il~(x~ii). Since IIZ’(O)I\ = 0, in a sufficiently small neighborhood of the origin we have /IT(x)!: 5
hence it will in turn suffice to prove that (Lo,, L(a, - CT,)), --t 0 as m, n -+ 30. Now
;jLlS’i2 = 2J(a,) is bounded, hence l\L(cr, - a,)/,, is bounded, and since L,_ - P,_h(cs,)
+ 0 in H,(Z, R”) it will suffice to prove that (P,,“/r(cr,) .L(c, - a,)), + 0 as tn. n -+ co.
Recalling that 0, - CJ,,, E H:(I, R”) (Theorem (I 1) of 913) it follows from Theorem (4)
above and Theorem (2) of $13 that
Jo
and since /Iu, - ornlln -+ 0 it will suffice to prove that
s ; I, Qo.(M~,)(~) II dt
is bounded. Let A be a compact set such that a,(J) c A
the fact that {a.} being uniformly Cauchy is uniformly
exists K such that f’
(the existence of A follows from
bounded). By the lemma there
-_
J IIQJ0h(~,)(~>li dt I KllL~,liollN~,)llo. 0
Now it has already been noted that IILa,jl, is bounded, and since
is j:h(o,) Ilo.
ilLa, - hi:, --, 0 so
q.e.d.
For the sake of completeness we give here a brief description of the classical conditions
that the critical points of J be non-degenerate and of a geometrical form of the Morse
Index Theoremt.
Let E denote the exponential map of V, into Y; i.e. if z: E V, then E(t.) = a( i/nl/)
where cr is the geodesic starting from P with tangent vector r*//ir’/. Then E is a Ck+2-map.
Given u E V, define n(v) = dimension of null-space of dE,. If I.(c) > 0 we call u a conjugate
vector at P. A point of V is called a conjugate point of P if it is in the image under E of
t For a detailed exposition the reader is referred to I. M. Singer’s Nofes on Di’rentiol Geometrv (Mimeographed, Massachusetts Institute of Technology. 1962).
332 RICHARD S. PALAiS
the P. By an easy special case of Sard’s Theoremt the set of
conjugate points of P has measure zero and in particular is nowhere dense in V.
Given u E E-‘(Q) define i; E n( V; P, Q) by t’(t) = E(t(c)). Then i; is a geodesic
parameterized proportionally to arc length (the proportionality factor being ;$;I), hence a
critical point of J by corollary of Theorem (5>, and conversely by the same corollary any
critical point of J is of the form v’ for a unique tr E E-‘(Q).
Non-degeneracy Theorem
If v E E-‘(Q) then ii is a degenerate point of J and only if is a
cector P, hence has only non-degenerate critical points lf and only if Q is not a conjugate
point of P. Itfollolvs that if Q is chosen outside a set of measure zero in V then J : fl( V; P, Q)
+ R has only non-degenerate critical points.
Morse Index Theorem
Let v E E- '(Q). Then there are only a finite number off sarisfying 0 < t < 1 such that
tr is a conjugate vector at P and the index of i; = 1 A(tv). In particular each critical point o<r< 1
of J : !2( V; P, Q) + R has finite index.
$15. TOPOLOGICAL IMPLICATIONS
Until now we have given no indication of why one would like to prove theorems such
as the Main Theorem. Roughly speaking the answer is that as a consequence of the Main
Theorem one is able to derive inequalities relating the number of critical points of a given
index with certain topological invariants of the manifold on which the function is defined.
These are the famous Morse Inequalities and are useful read in either direction. That is,
if we know certain facts about the topology of the manifold they imply existential statements
about critical points, and conversely if we know certain facts about the critical point
structure we can deduce that the topology of the manifold can be only so compli-
cated.
As a start in this direction we will show that if M is a complete C2-Riemannian
manifold and f: M + R is a C2-function bounded below and satisfying condition (C) then
on each component of Mf assumes its lower bound. Note that we do not assume that the
critical points off are non-degenerate, however since it is clear that a point where f assumes
a local minimum is a critical point, and is of index zero if non-degenerate, it follows that
if the critical points off are all non-degenerate then there are at least as many critical points
of index zero as there are components of M. This is the first Morse inequality.
In what follows we denote the frontier of a set K by R.
THEOREM (1). Let M be a connected Cl-manifoldf: M + R a non-constant C’-function
and K the set of critical points ofJ Then f(K) = f(k).
t DE RHAM: Variete’s Difirentiable, p. 10.
MORSE THEORY ON HILBERT MANIFOLDS 333
Proof. Let p E K. We will find x E k such that f(x) = f(J). Choose q E M with
.fiq) #f(p) and G : I + M a Cl-path such that a(0) = p and a( 1) = q and let g(t) = f(b(t)).
Then g’(t) = dfec,,(b’(r)) and since g is not constant. g’ is not identically zero, so a(I) is
not included in K. Let t, = Inf{t E Ila(t) $ Ki. Then x = o(r,) E k and since g’(r) = 0
for 0 I I I fO.f(s) = g(LO) = g(0) = f(p).
q.e.d.
THEOREM (2). Let M be u Cl-Riemanniun manifold, f: M + R a C’-function
satisfving condition (C) and K the set of critical points of f. Then f Ik is proper;
i.e. gicen - x < a < h < x. h; n f - ‘([a, b]) is compact (note rcle do not assume that M
is complete).
Proof. Let (p,) be a sequence in ti with II I .fp,) 5 6. Since h’ is closed it will suffice
to prove that {p,) has a convergent subsequence. Since p, E fi we can choose q. $ K
arbitrarily close to p,. In particular since ;Vf is continuous and ~ Vf,,i! = 0 we can
choose q, so close to p, that
llVfb.ll < d 7 a - 1 <j(qn) < b + I
and also
1 P(4.* P”) < ;
where p is the Riemannian metric for M. Then by condition (C) a subsequence of {q.} will
converge to a critical point p off. Since
the corresponding subsequence of {II,) will also converge to p. q.e.d.
Remark. f IK need not be proper-for example if M is not compact and f is constant
then f trivially satisfies condition (C) and K = M. -_
THEOREM (3)t. Let M be a complete C”-Riemannian manifold without boundary,
f: M + R a C2-function satisfying condition (C) and 0 : (r, ,Ll) - M a maximum integral
curre of VJ Then either lim f(a(t)) = co or else /I = 00 and D(I) has a critical point off
as a limit point as t --+ co. Similarly either lim f(o(t)) = -co or else z = -m and o(t)
has a critical point off as limit point as t --t - SO.
Proof. This is just the lemma to Proposition (2) of $10 restated verbatim. We simply
note that in the proof of that lemma we did not use the standing assumptions of $10 that f
was C3 or that the critical points off were non-degenerate.
THEOREM (4). Let M be a complete C2-Riemannian man[fold and f: M -+ R a C2-
function satisfying condition (C). [ff b IS ounded below on a component M, of M then f IM,
assumes its greatest lower bound.
t In this regard see also Proposition (3) of $12.
334 RICHARD S. PALAIS
Proof. We can assume that A4 is connected. Let B = Inf{f(x)l.r E ,t!). Given E > 0
choose p E M such that_@) < B + E. If d : (z, /?) 4 M is the maximum integral curve of
Vfwith initial condition p then by Theorem (3) r = - x and ~$1) has a critical point q as
limit point as t -+ -co. Since f(a(t)) is monotonic non-decreasingf(:q) < B + E. Since
the theorem is trivial iffis constant we can assume f is not constant and it follows from
Theorem (1) that if K is the set of critical points off we can find x in E(‘, the frontier of K,
such thatf(x) < .B + E. Choose x, E R such that
Blf(X,) < B + ‘. n
Then by Theorem (2) a subsequence of {x,1 will converge to a point x and clearly,f(x) = B.
q.e.d.
COROLLARY (1). If the set of critical points off has no interior and iff’is hounded be/o,\*
an ,bf then f assumes its greatest IoH-er bound.
Proof. If B is the greatest lower bound off then for every positive integer n we can
choose x, E h; (a minimum off on some component of M) such that
Since K has no interior and is closed K = R, so by Theorem (2) a subsequence of {x,} will
converge to a point x wheref(x) = B.
q.e.d.
COROLLARY (2). If V is a C6 complete Riemannian man/fold and P. Q E V then [he
action integral J” assumes its greatest lolc*er bound on each component qf R(V; P, Q) and
also on i2( V; P, Q).
Proof. We saw in Theorem (6) of 914 that condition (C) is satisfied. If K is the set of
critical points of J”IR( V; P, Q) then by the corollary of Theorem (5) of $14 the elements c
of K are (geodesics) parameterized proportionally to arc length. By making a small para-
meter change we can get element of R(V; P, Q) arbitrarily close to 0 which are not
parameterized proportionally to arc length, hence K has no interior.
Remark. If V is a complete Riemannian manifold and P, Q E V then given an abso-
lutely continuous path 0 : I + I/ with a(O) = P, a(l) = Q define the length of 6, L(U), by
L(c) = iijcr’(l)ii dt. s 0
Then by Schwartz’s inequality if G E fi( V; P, Q) L(O) I (W(G))“’ and moreover equality
occurs if and only if 116 /I is constant, i.e. if and only if 0 is parameterized proportionally to
arc length. Now if CT : I --+ V is absolutely continuous and a(0) = P, o(l) = Q we can
reparameterize d proportionally to arc length, getting y : I -+ V. Then y E 0( V; P, Q) and since
arc length is independent of parameterization L(y) = L(a). Since reparameterizing also does
not affect the homotopy class of u we see that if J” assumes its greatest lower bound on a
component of fi( V; P, Q) at a point y (SO that y is a geodesic parameterized proportionally
MORSE THEORY ON HILBERT MAMFOLDS 335
to arc length) then among all absolutely continuous paths joining P to Q and homotopic
to 7, 7 has the smallest length. Together with the preceding corollary this gives:
THEOREM (5). If V is a complete C6-Riemannian manifald. P, Q E V then gicen an>
homotop>, class of paths joining P E Q there is a geodesic in this class rc,hose length is less than
or equal to that of any other absolutely continuous path in the class. Moreowr there is a
geodesic joining P to Q rc,hose length is p(p, q).
Let Hi be a Hilbert space of dimension di. i = 1, . . . . n, D, the closed unit disc in Hi and
Si the unit sphere in Hi. Let gi : Si -+ X be continuous maps with disjoint images in a
topological space X. We form a new space X ug, D, u . up, D, (called the result of
attaching cells of dimension d,, ,.., d, to X by attaching maps gr, . . . . gn) by taking the
topological sum of X and the Di and identifying y E Di with gi(y) E X. Suppose now that
di < w i = I. . . . . m and di = m i > m. Then X ug, D, u . ug, D, is a strdng de-
formation retract of X u,, D, u . . . uy, D,. It will suffice to prove that if D is the unit
disc and S the unit sphere in a Hilbert space H of infinite dimension then S is a strong
deformation retract of D, or since D is convex it will suffice to find a retraction p : D + S.
By a theorem of Klee [2.2 of 31 there is a fixed point free map h : D -+ D (to see this note
that if {.Y,:-,~~ is a complete orthonormal basis for H then
f(f) = (
cos VI,. + (sin v)x”+, ,IIt<!lfl
defines a topological embedding of R onto a closed subset F of D. Since F is an absolute
retract the fixed point free map f(t) -f(t + 1) of F into F can be extended to a map
h : D + F which is clearly fixed point free). We define p : D + S by p(x) = point where the
directed line segment from h(x) to .Y meets S.
It now follows (by excision) that if H, denotes the singular homology functor with any coefficient group G then
H,(A’ u,, D, u ug,, D,. A’) z ic,H,(D”z. Sd8-‘)
hence for any positive integer r
H,(X ug, D, u . . . u,,, D,, X) = G p’r’
--
where p(r) is the number of indices i = I. _.,, n such that di = r.
Next let N be a Hilbert manifold with boundary and suppose M arises from N by
disjoint C-attachments (Jr, . . . . f,) of handles of type (d,, el), . . . . (d,, e,) ($11). Define
attaching maps gi : Sdi- ’ -+ dN by gi(y) = fi(y, 0). (Note that since f, : Ddi x D” -+ M
is a homeomorphism each gi is a homeomorphism.) Then clearly N ufr( Ddl x 0) u . . ufXDd' x 0) can be identified with N ug, D”’ u . ugn Dd”. We shall now prove that
Nu ;/,(D”%O) i=l
is a strong deformation retract of M, hence by what we have just proved above that if
di < 00 i = 1, . . . . m, di - CO i > m then Nu,, Dd’ u . . . ug Dd” is a strong deformation
336 RICHARDS. PALAIS
retract of M. It will suffice to prove that (od x 0) u (Sd-’ x D’) is a strong deformation
retract of D“ x D’, and since D“ x D’ is convex it will suffice to define a retraction r of
D“ x D’ onto (od x 0) u (Sd-’ x 0’). Deiine r(x, 0) = (x, 0) and if y # 0 define
dx,_V)= (j-$-jjj,O) if l/xl/ 51 -y
4x,L’)= ( & WI + /IY// - 2) & ) if Ijx// 2 1 -u 2 .
From the above remarks together with the theorem of $12 we deduce:
THEOREM (6). Let M be a complete C3-Riemannian manifold, f: M -+ R a C3-function
satisfying condition (C) all of whose critical points are non-degenerate, c a critical value off.
pl, . ., pn the critical points of finite index on the level c, and let di be the index of pi. If
c is the only critical tlalue off in a closed interral [a, b] then M, has as a deformation retract
M, with cells of dimension d,, . .., d, disjointly attached to S,M, by homeomorphisms of the
boundary spheres. Hence if Hk denotes fhe singular homology funcfor in dimension k with
coeficient group G then H,(M,, M,) z G”” where C(k) is the number of critical points of
index k on the lecel c.
Remark. The surprising fact about Theorem (6) is that the homotopy type of(M,, M,)
depends only on the critical points of finite index on the level c, those of infinite index being
homotopically invisible. This is of course just a reflexion of the theorem of Klee that the
unit disc modulo its boundary in an infinite dimensional Hilbert space is homotopically
trivial. If it were not for this unexpected phenomenon we would have to make the rather
unaesthetic assumption that all critical points were of finite index in order to derive Morse
Inequalities.
In deriving the Morse Inequalities we shall follow Milnor closely. Let F denote a
fixed field and H, the singular homology functor with coefficients F. We call a pair of
spaces (X, Y) admissible if H,(X, Y) is of finite type, i.e. each H,(X, Y) is finite dimensional
and H,(X, Y) = 0 except for finitely many k. From the exact homology sequence of a
triple (X, Y, 2) it follows that if (X, Y) and ( Y, 2) are admissible then so is (A’, Z). We
call an integer valued function S on admissible pairs subadditive if %A’, Z) I S(X, Y) +
S( Y, Z) for all triples (X, Y, Z) such that (X, Y) and ( Y, Z) are admissible, and S is called
additive if equality always holds in the above inequality. Then by an easy induction if
X,, 2 A’,_, 2 . . . 2 A’, and each (Xi+r, Xi) is admissible it follows that (X,, X,-J is
admissible and n--l
S(x,, x0) 5 1 S(xi+ 1, xi) i=O
if S is subadditive, equality holding if S is additive.
DEFINITION. For each non-negative integer k we define in!eger ralued functions R, and
S, on admissible pairs by R,(X, Y) = dim Hk(X, Y) and
S,(X, Y) = c (- l)k_“R,(X, Y). mzzk
MORSE THEORY ON HILBERT MANIFOLDS 337
We define the Euler characteristic x for admissible pairs bj
x(X, Y) = f (- l)“R,(X, Y). m=O
LEMMA. R, and S, are subadditire and x is additire.
Proof. Let (X, Y, Z) be a triple of spaces such that (X, Y) and (Y, Z) are admissible.
From the long exact homology sequence of the triple (X, Y, Z)
i, im + H,( Y, Z) + H,(X, 2) + H,(X-, Y) “1 H,_ L( Y, Z) -+
we derive the usual three short exact sequences
O+im(~,+,)-+H,(Y, Z)-im(i,) -+O
O-+ im(i,) - H,(X, Z) ---) im(j,) -+ 0
0 --+ im(j,) - H,(X, I’)-im(ci,)-+O
from which follow
R,(Y, Z) = dim H,(Y, Z) = dim im(d,+ ,) + dim im(i,)
If we multiply (,) by (- l)k-m and sum over m from m = 0 to m = k we get
S,(X, Z) - S,(X, Y) - S,(Y, Z) = (-I)‘+’ dim im(S,) - dim im(d,+,)
which is negative since in fact do = 0. Similarly if we multiply (,) by (- I)” and sum over
all non-negative m we get x(X, Z) - z(X, Y) - x( Y, Z) = 0 since zk+ I = 0 for k
sufficiently large.
-q.e.d.
Now letfand A4 be as in Theorem (6). Let - co < a < b < CL) and suppose a and b
are regular values off: Let cr, . .., c, be the distinct critical values offin [a, b] in increasing
order. Choose a,, i = 0, . . . . nsothata = a, < c, < a1 < c2 < . . . < a,_, < c, < a, = b
and put Xi = M,, = {x E MIf(x) I a,}. Then by Theorem (6) (Xi+rr Xi) is admissible
and Rk(Xi+r, Xi) = number of critical points of index k on the level ci. Hence
sk(xi+l,~~i) =m~o(-l)k-m ( number of critical points of index m on level ci)
and
Axi+ 19 xi> = number of critical points of index m on the level ci).
Hence .
n-l
~osk(xi+l~ xJ =m~oC-l)k-m ( number of critical points of index m inf -‘([a, b])
338 RICHARDS. PALAIS
while
n-1
i&oX(xi+ 13 xi) = f (- l)” ( number of critical points of index m in ~-‘([a, b]) m=O
Since Sk and x are subadditive and additive respectively we deduce
THEOREM (7). (MORSE INEQUALITIES.) Let M be a complete C’-Riemannian manifold,
f:M+RaC3-f t’ unc ran satisfying condition (C) all of whose critical points are non-degenerate.
Let a and b be regular values ofJ a < 6. For each non-negatire integer M let R, denote the
mth betti-number of (Mb, M,) relative to somejixedfield F and let C, denote the number of
critical points off of index m in f - ‘([a, b]). Then
R, 5 Co
and
R, - R, < C, - Co
,jo(- l)k-mR, 2 m$o(- I)‘-“&
x(kI,, M6) = f (- l)“R, = i (- l)“C,. m=O m=O
COROLLARY (1). R, I C, for all m.
COROLLARY (2). Iff is bounded below then the conclusions of the theorem and of Corollary
(1) remain valid if we interpret R, = mth betti-number of M, and C,,, = number of critical
points off having index m in Mh respecticely.
Proof. Choose a < glb J
COROLLARY (3). If f is bounded belorct then for each non-negatire integer m Rz I Cz,
where Rz is the mth betti-number of M and C,* is the total number of critical points off having
index m. (Of course either or both of Rz and C,* may be infinite.) -
Proof. By Corollary (2) we have C’z L R,(M,) for any regular value b off. Hence it
will suffice to show that if Rz = dim H,(M; F) 2 k for some non-negative integer k then
R,(M,) r k for some regular value b off. Let h,, . . . . h, be linearly independent elements
of H,,,(M; F), Z1, . . . . zk singular cycles of M which represent them, and C a compact set
containing the supports of z,, . . . . z,. Then as b + CO through regular values off the
interiors of the Mb form an increasing family of open sets which exhaust M, hence C c M,
for some regular value b of J Then zI, . . . . ;k are singular cycles of Mb, moreover no
non-trivial linear combination of them could be homologous to zero in M, since that same
combination would a fortiori be homologous to zero in M. Hence R,(M,) 2 k. q.e.d.
Caution. The assumption that f is bounded below is necessary in Corollary (3) as can
be seen by considering the identity map of R which has no critical points even though
R;(R) = 1.
We refer the reader to [8] for more delicate forms of the Morse Inequalities.
MORSE THEORY 0% HILBERT 41ASIFOLDS 339
Remark. If k’ is a complete C6-Riemannian manifold, P, Q E V define Q,,o( V) to be
the set of continuous maps cr : I + V such that a(O) = P and a(l) = Q, in the compact
open topology. The standard techniques of homotopy theory relate the topology of V and
that of fZ?,,,( V), while Theorem (7) and the results of $13 together give results concerning
the topology of n( V; P, Q). Clearly some sort of bridge theorem relating Q,,,(V) and
f2( k’; P, Q) is desirable. Now if V is imbedded as a closed submanifold of R” then
fZ( I’; P, Q) is a closed submanifold of H,(I, R”). While R,.o( k’) is a subspace of C”(Z, R”),
hence it follows from Corollary (2) of Theorem (3) ($13) that the inclusion map
i : C.l( b’; P, Q) 3 fi,,,( V) is continuous. The desired bridge theorem is the statement that
i is in fact a homotopy equivalence. A homotopy inverse can be constructed by using
smoothing operators of convolution type.
i:f !I: = s’i f(x) j2 du(x)
on the space CO(D”, R”) of CD-maps
( w h ere u is Lebesque measure on D”)
and
IlJiC = , EkllFfiiL I
Then the completion of C%(D”, R”) relative to the norm Ij IIL is a Hilbert space which we
denote by H,(D”, R”). We denote by H:(D”, R”) the closure in H,(D”, R”) of the set of
f in Cp( D”, R”) such that (WY)(x) = 0 if x E S”-’ and 121 I k - 1. Let V be closed
C”-submanifold of R” and let Hk( D”, V) = {f~ H,(D”, R”)IF(D”) c Y}. Ifg E H,.(D”, V) we define fY( V; g) = {f E H,(D”, V)jf - g E H:(D”, R”)}. It follows from the Sobolev
Inequalities that if 2k > n Hk( D”, V) and fY( V; g) are closed submanifolds of the Hilbert
space HK( D”, R”). More generally analogous Hilbert manifolds of HK maps of Miiito V’
can be constructed for any compact C” n-manifold with boundary M replacing D’. Note
that for k = II = 1, H,(D’, V) = H,(/, V) and fJ’(V,g) = n(V;g(O),g(l)). A question
that immediately presents itself is to find functions J : !A”( V; g) 4 R which are analogues
of the action integral and satisfy condition (C). If A is a strongly elliptic differential operator
of order 2k then J(f) = -) (AL f >. is such a good analogue of the action integral provided
_4f = 0 has no solutions f in Hc( D”, R”). In particular if L is an elliptic kth order elliptic
operator such that Lf = 0 has no solutions f in H:(D”, R”) then J(f) = +l/Lf 11; =+
(L*LJ, f ). is such a function (taking k = n = 1 and L = d/dt gives the ordinary action
integral). Smale has found an even wider class of functions which also satisfy condition (C).
Now let n < m and regard O(n) 5 O(m) in the standard way. Define an orthogonal
representation of O(n) on HJD”, R”) by (T/)(x) = T(f (T-*x)). If we take V = Sm-’ then
since V is invariant under O(n) it follows that H,(D”, V) is a invariant submanifold of
H,(D”, R”). Moreover if we define g E H,.(D”, V) by g(x) = (x,, . . . . x,, \/I - llx/!‘, 0 . . . 0)
then Tg = g for any T E O(n) and it follows that fY( k’, g) is also an invariant submanifold
330 RICHARD S. PALAlS
of H,(D”, Y), hence O(n) is a group of isometries of the complete Riemannian manifold
n”(Y, g). Now suppose A is a strongly elliptic differential operator of order 2k,
A : C”(D”, R”) -+ Cr(Dn, R”), such that A(Tf) = T(.4f) for all TE O(n), for example
A = Ak where A is the Laplacian
ii, 2.
Then J:R(V,g) 4 R defined by J(f) = +<Ai_f>,, satisfies J( 7f‘) = f for any T E O(U).
hence iffis a critical point of J so is rffor any TE O(n). and since non-degenerate critical
points of J are isolated, Tf = f if f is a non-degenerate critical point of J. But Tf = _/‘ is
equivalent to R(f(.r)) being a function F of ‘jxll where R is the distance measured along the
sphere .S”- ’ = V of a point on I/ to the north pole. Moreover F will satisfy an ordinary
differential equation of order 2k. With a little computation one should be able to compute
all the critical points and their indices and hence, via the Morse inequalities, get information
about the homology groups of f2”(V, g) (which has the homotopy type of the nth loop
space of .S”- ’ ). Clearly the same sort of process will work whenever we can force a large
degree of symmetry into the situation.
REFERENCFS
I. J. DIEUDONNE: Foundurions of Mondern Analysis. Academic Press, New York, 1960. 2. J. EELLS: On the geometry of function spaces, Symposium Inrernacional de Topolo,qia A!quhraica (,Me.riw.
1956), pp. 303-308. 1958. 3. V. KLEE: Some topological properties of convex sets, Trans. Amer. Marh. Sot. 78 (1955). 30-45. 4. S. LANG: Introduction to Differentiable Manifolds, Interscience, New York, 1962. 5. J. MILNOR: Morse theory, Ann. Math. Sud. No. 51, (1963). 6. M. MORSE: The calculus of variations in the large. Colloq. Lect. Amer. Math. Sot. 18 (1933). 7. J. NA.SH: The imbedding problem for Riemannian manifolds, Ann. Mafh., Princeton 63 (1956). 20-63 8. E. PITCHER: Inequalities of critical point theory, Bull. Amer. r2fanth. Sot. 64 (1958). I-30.